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| | *A shift matrix U with ones on the superdiagonal is an upper shift matrix. | | *A shift matrix U with ones on the superdiagonal is an upper shift matrix. |
| | *The alternative subdiagonal matrix L is unsurprisingly known as a lower shift matrix. | | *The alternative subdiagonal matrix L is unsurprisingly known as a lower shift matrix. |
| − | *Let Z is a shift matrix , then ZA, ZTA, AZ, AZT, ZAZT are equal to the matrix A shifted one position down, up left, right, and down along the main diagonal respectively. | + | *Let Z is a shift matrix , then <math>ZA, Z^TA, AZ, AZ^T, ZAZ^T</math> are equal to the matrix A shifted one position down, up left, right, and down along the main diagonal respectively. |
| | *The alternative subdiagonal matrix L is unsurprisingly known as a lower shift matrix. | | *The alternative subdiagonal matrix L is unsurprisingly known as a lower shift matrix. |
| − | *The (i,j):th component of U and L are | + | *The <math>(i,j)^th</math> component of U and L are |
| − | U_{ij} = \delta_{i+1,j}, \quad L_{ij} = \delta_{i,j+1},where \delta_{ij} is the Kronecker delta symbol. | + | <math>U_{ij} = \delta_{i+1,j}, \quad L_{ij} = \delta_{i,j+1}</math>,where <math>\delta_{ij}</math> is the Kronecker delta symbol. |
| | *For example, the 5×5 shift matrices are: | | *For example, the 5×5 shift matrices are: |
| | *All shift matrices are nilpotent; an n by n shift matrix S becomes the null matrix when raised to the power of its dimension n. | | *All shift matrices are nilpotent; an n by n shift matrix S becomes the null matrix when raised to the power of its dimension n. |